The main result of [1]} is the following pointwise decay, which captures the so-called Price law for fixed
angular momentum. Strictly speaking, it is still off by one power of \(t\)  from the sharpest
form of Price's law which is \(t^{-2\ell -3}\)  whereas the following result proves \(t^{-2\ell -2}\) 
(we shall comment on that issue below). Note how the accelerated decay for higher values of \(\ell \)  mirrors
what we saw for the surfaces of revolution in Theorem REF . Hintz [2]} recently closed the gap of the missing power of \(t\)  and thus finished the proof of Price's law.
